1. Thermodynamics Chapter 10
Section 1 Relationships Between Heat and Work
Chapter 10
Thermodynamics

2. Section 1 Relationships Between Heat and Work
Chapter 10
Objectives
Recognize that a system can absorb or release energy as heat in order for work to be done on or by the system and that work done on or by a system can result in the transfer of energy as heat.
Compute the amount of work done during a thermodynamic process.
Distinguish between isovolumetric, isothermal, and adiabatic thermodynamic processes.

3. Heat, Work, and Internal Energy
Section 1 Relationships Between Heat and Work
Chapter 10
Heat, Work, and Internal Energy
Heat and work are energy transferred to or from a system. An object never has “heat” or “work” in it; it has only internal energy.
A system is a set of particles or interacting components considered to be a distinct physical entity for the purpose of study.
The environment the combination of conditions and influences outside a system that affect the behavior of the system.

4. Heat, Work, and Internal Energy, continued
Section 1 Relationships Between Heat and Work
Chapter 10
Heat, Work, and Internal Energy, continued
In thermodynamic systems, work is defined in terms of pressure and volume change.
This definition assumes that P is constant.

5. Heat, Work, and Internal Energy, continued
Section 1 Relationships Between Heat and Work
Chapter 10
Heat, Work, and Internal Energy, continued
If the gas expands, as shown in the figure, DV is positive, and the work done by the gas on the piston is positive.
If the gas is compressed, DV is negative, and the work done by the gas on the piston is negative. (In other words, the piston does work on the gas.)

6. Heat, Work, and Internal Energy, continued
Section 1 Relationships Between Heat and Work
Chapter 10
Heat, Work, and Internal Energy, continued
When the gas volume remains constant, there is no displacement and no work is done on or by the system.
Although the pressure can change during a process, work is done only if the volume changes.
A situation in which pressure increases and volume remains constant is comparable to one in which a force does not displace a mass even as the force is increased. Work is not done in either situation.

7. Thermodynamic Processes
Section 1 Relationships Between Heat and Work
Chapter 10
Thermodynamic Processes
An isovolumetric process is a thermodynamic process that takes place at constant volume so that no work is done on or by the system.
An isothermal process is a thermodynamic process that takes place at constant temperature.
An adiabatic process is a thermodynamic process during which no energy is transferred to or from the system as heat.

8. Chapter 10 Energy Conservation
Section 2 The First Law of Thermodynamics
Chapter 10
Energy Conservation
If friction is taken into account, mechanical energy is not conserved.
Consider the example of a roller coaster:
A steady decrease in the car’s total mechanical energy occurs because of work being done against the friction between the car’s axles and its bearings and between the car’s wheels and the coaster track.
If the internal energy for the roller coaster (the system) and the energy dissipated to the surrounding air (the environment) are taken into account, then the total energy will be constant.

9. Chapter 10 Energy Conservation
Section 2 The First Law of Thermodynamics
Chapter 10
Energy Conservation

10. Energy Conservation, continued
Section 2 The First Law of Thermodynamics
Chapter 10
Energy Conservation, continued
The principle of energy conservation that takes into account a system’s internal energy as well as work and heat is called the first law of thermodynamics.
The first law of thermodynamics can be expressed mathematically as follows:
DU = Q – W
Change in system’s internal energy = energy transferred to or from system as heat – energy transferred to or from system as work

11. Signs of Q and W for a system
Section 2 The First Law of Thermodynamics
Chapter 10
Signs of Q and W for a system

12. Chapter 10 Sample Problem The First Law of Thermodynamics
Section 2 The First Law of Thermodynamics
Chapter 10
Sample Problem
The First Law of Thermodynamics
A total of 135 J of work is done on a gaseous refrigerant as it undergoes compression. If the internal energy of the gas increases by 114 J during the process, what is the total amount of energy transferred as heat? Has energy been added to or removed from the refrigerant as heat?

13. Sample Problem, continued
Section 2 The First Law of Thermodynamics
Chapter 10
Sample Problem, continued
1. Define
Given:
W = –135 J
DU = 114 J
Diagram:
Tip: Work is done on the gas, so work (W) has a negative value. The internal energy increases during the process, so the change in internal energy (DU) has a positive value.
Unknown:
Q = ?

14. Sample Problem, continued
Section 2 The First Law of Thermodynamics
Chapter 10
Sample Problem, continued
2. Plan
Choose an equation or situation:
Apply the first law of thermodynamics using the values for DU and W in order to find the value for Q.
DU = Q – W
Rearrange the equation to isolate the unknown:
Q = DU + W

15. Sample Problem, continued
Section 2 The First Law of Thermodynamics
Chapter 10
Sample Problem, continued
3. Calculate
Substitute the values into the equation and solve:
Q = 114 J + (–135 J)
Q = –21 J
Tip: The sign for the value of Q is negative. This indicates that energy is transferred as heat from the refrigerant.